% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 37346 % Primary Name: OLNEYVILLE % Record Type: TAVG % Country: United States % State: RI % Latitude: 41.80000 +/- 0.00005 % Longitude: -71.48330 +/- 0.00005 % Elevation (m): 47.68 +/- 50.06 % # of Months: 8 % % Alternate Names: Missing Station ID - 375610 % % IDs: coop - 375610 % ghcnd - USC00375610 % ncdc - 12004873 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 347438240147f84acacc6b654d3bfc16 % Raw Data Hash: 1ee0131ebcc74ad13c4179394240573a % Adj Data Hash: 80372473fcabc00ccce66f2c28d52c7c % % The data for this station is presented below in several columns and in % several forms. The temperature values are reported as "raw", % "adjusted", and "regional expectation". % % The "raw" values reflect the observations as originally ingested by % the Berkeley Earth system from one or more originating archive(s). % These "raw" values may reflect the merger of more than one temperature % time series if multiple archives reported values for this location. % Alongside the raw data we have also provided a flag indicating which % values failed initial quality control checks. A further column % dates at which the raw data may be subject to continuity "breaks" % due to documented station moves (denoted "1"), prolonged measurement % gaps (denoted "2"), documented time of observation changes (denoted "3") % and other empirically determined inhomogeneities (denoted "4"). % % In many cases, raw temperature data contains a number of artifacts, % caused by issues such as typographical errors, instrumentation changes, % station moves, and urban or agricultural development near the station. % The Berkeley Earth analysis process attempts to identify and estimate % the impact of various kinds of data quality problems by comparing each % time series to neighboring series. At the end of the analysis process, % the "adjusted" data is created as an estimate of what the weather at % this location might have looked like after removing apparent biases. % This "adjusted" data will generally to be free from quality control % issues and be regionally homogeneous. Some users may find this % "adjusted" data that attempts to remove apparent biases more % suitable for their needs, while other users may prefer to work % with raw values. % % Lastly, we have provided a "regional expectation" time series, based % on the Berkeley Earth expected temperatures in the neighborhood of the % station. This incorporates information from as many weather stations as % are available for the local region surrounding this location. Note % that the regional expectation may be a systematically a bit warmer or % colder than the weather stations by a few degrees due to differences % in mean elevation and other local characteristics. % % For each temperature time series, we have also included an "anomaly" % time series that removes both the seasonality and the long-term mean. % These anomalies may provide an easier way of seeing changes through % time. % % Reported temperatures are in Celsius and reflect monthly averages. As % these files are intended to be summaries for convenience, additional % information, including more detailed flagging and metadata, may be % available in our whole data set files. % % The Berkeley Earth analysis was run on 15-Nov-2013 19:55:48 % % Raw Data QC Continuity Adjusted Data Regional Expectation % Year, Month, Temperature, Anomaly, Failed, Breaks, Temperature, Anomaly, Temperature, Anomaly 1892 1 NaN NaN NaN NaN NaN NaN -5.608 0.137 1892 2 NaN NaN NaN NaN NaN NaN -4.690 -0.023 1892 3 NaN NaN NaN NaN NaN NaN -1.887 -2.470 1892 4 NaN NaN NaN NaN NaN NaN 6.668 -0.338 1892 5 NaN NaN NaN NaN NaN NaN 11.756 -1.477 1892 6 NaN NaN NaN NaN NaN NaN 19.636 1.341 1892 7 NaN NaN NaN NaN NaN NaN 20.731 -0.256 1892 8 NaN NaN NaN NaN NaN NaN 19.502 -0.327 1892 9 NaN NaN NaN NaN NaN NaN 14.400 -1.032 1892 10 NaN NaN NaN NaN NaN NaN 8.379 -1.018 1892 11 NaN NaN NaN NaN NaN NaN 2.808 -0.861 1892 12 NaN NaN NaN NaN NaN NaN -5.351 -2.012 1893 1 -4.837 -2.228 1 0 NaN NaN -10.011 -4.266 1893 2 NaN NaN NaN NaN NaN NaN -6.301 -1.634 1893 3 NaN NaN NaN NaN NaN NaN -1.588 -2.171 1893 4 NaN NaN NaN NaN NaN NaN 4.902 -2.104 1893 5 13.491 -2.877 0 0 13.491 -2.877 12.433 -0.800 1893 6 19.341 -2.089 0 0 19.341 -2.089 18.205 -0.090 1893 7 21.832 -2.290 0 0 21.832 -2.290 19.858 -1.129 1893 8 21.461 -1.503 0 0 21.461 -1.503 19.427 -0.401 1893 9 16.393 -2.174 0 0 16.393 -2.174 12.676 -2.756 1893 10 15.068 2.535 0 0 15.068 2.535 10.091 0.693 1893 11 9.933 3.129 0 0 9.933 3.129 2.884 -0.785 1893 12 NaN NaN NaN NaN NaN NaN -5.172 -1.833 1894 1 NaN NaN NaN NaN NaN NaN -4.561 1.183 1894 2 NaN NaN NaN NaN NaN NaN -6.819 -2.152 1894 3 NaN NaN NaN NaN NaN NaN 3.336 2.753 1894 4 NaN NaN NaN NaN NaN NaN 7.065 0.059 1894 5 NaN NaN NaN NaN NaN NaN 13.058 -0.175 1894 6 NaN NaN NaN NaN NaN NaN 18.770 0.475 1894 7 NaN NaN NaN NaN NaN NaN 21.586 0.598 1894 8 NaN NaN NaN NaN NaN NaN 18.331 -1.498 1894 9 NaN NaN NaN NaN NaN NaN 16.350 0.918 1894 10 NaN NaN NaN NaN NaN NaN 9.441 0.044 1894 11 NaN NaN NaN NaN NaN NaN 0.934 -2.735